
A capillary tube of radius ‘r’ is lowered into a liquid of surface tension, T and density, \[\rho \]. The work done by surface tension when the angle of contact is \[{{0}^{0}}\] -
\[\begin{align}
& A)\text{ }\dfrac{\pi {{T}^{2}}}{\rho g} \\
& B)\text{ }\dfrac{4\pi {{T}^{2}}}{\rho g} \\
& C)\text{ }\dfrac{{{T}^{2}}}{\rho g} \\
& D)\text{ }\dfrac{2{{T}^{2}}}{\rho g} \\
\end{align}\]
Answer
563.4k+ views
Hint: We need to find the height of the capillary tube that is immersed in the liquid. From the height given we can calculate the work done by using proper relations. The height can be found using the equation for the surface tension with density term.
Complete answer:
Surface tension is the force acting on the liquid at the place of contact with another medium per unit length. It is also defined as the surface energy or the work done by the liquid per unit area of the liquid. The point of contact plays an important role in the surface energy. The angle of contact determines whether the two media is attracted to each like water on a glass or repelled like mercury on glass.
Let us see how we can find the work done by the liquid in the capillary tube from the given data.
\[\begin{align}
& \text{Surface tension, T}=\dfrac{F}{2\pi r\cos \theta } \\
& \Rightarrow \text{ }F=2\pi Tr\cos \theta \\
\end{align}\]
From the figure we can understand that
\[\begin{align}
& \theta ={{0}^{0}} \\
& \Rightarrow \text{ }\cos \theta =1 \\
& \therefore \text{ }F=2\pi Tr \\
\end{align}\]
Now, we can find the height of liquid in the capillary tube by equating the force due to air pressure and the surface tension as –
\[\begin{align}
& F=h\rho g\times \pi {{r}^{2}} \\
& \text{and,} \\
& F=2\pi rT \\
& \Rightarrow \text{ }h\rho g\times \pi {{r}^{2}}=2\pi rT \\
& \Rightarrow \text{ }\rho \pi {{r}^{2}}hg=2\pi rT \\
& \Rightarrow \text{ }h=\dfrac{2T}{\rho rg} \\
\end{align}\]
Now, we can find the work done by the liquid as –
\[\begin{align}
& \text{Work done = Surface tension}\times \operatorname{l}\text{length of contact}\times \text{height of liquid column} \\
& \Rightarrow \text{ }W=T\times 2\pi r\times \dfrac{2T}{\rho rg} \\
& \Rightarrow \text{ }W=\dfrac{4\pi {{T}^{2}}}{\rho g} \\
\end{align}\]
So, we have the work done by the liquid to reach at height ‘h’ as –
\[W=\dfrac{4\pi {{T}^{2}}}{\rho g}\]
The correct answer is given by option B.
Note:
We can find the work done by integrating the surface tension over the area of contact, i.e., in this case the area of the circular face of the capillary tube. We had to find the height in this problem as the options involved didn’t have the height in the equation of the work done.
The work done by the liquid in rising in a capillary tube is the work done against the air pressure.
Complete answer:
Surface tension is the force acting on the liquid at the place of contact with another medium per unit length. It is also defined as the surface energy or the work done by the liquid per unit area of the liquid. The point of contact plays an important role in the surface energy. The angle of contact determines whether the two media is attracted to each like water on a glass or repelled like mercury on glass.
Let us see how we can find the work done by the liquid in the capillary tube from the given data.
\[\begin{align}
& \text{Surface tension, T}=\dfrac{F}{2\pi r\cos \theta } \\
& \Rightarrow \text{ }F=2\pi Tr\cos \theta \\
\end{align}\]
From the figure we can understand that
\[\begin{align}
& \theta ={{0}^{0}} \\
& \Rightarrow \text{ }\cos \theta =1 \\
& \therefore \text{ }F=2\pi Tr \\
\end{align}\]
Now, we can find the height of liquid in the capillary tube by equating the force due to air pressure and the surface tension as –
\[\begin{align}
& F=h\rho g\times \pi {{r}^{2}} \\
& \text{and,} \\
& F=2\pi rT \\
& \Rightarrow \text{ }h\rho g\times \pi {{r}^{2}}=2\pi rT \\
& \Rightarrow \text{ }\rho \pi {{r}^{2}}hg=2\pi rT \\
& \Rightarrow \text{ }h=\dfrac{2T}{\rho rg} \\
\end{align}\]
Now, we can find the work done by the liquid as –
\[\begin{align}
& \text{Work done = Surface tension}\times \operatorname{l}\text{length of contact}\times \text{height of liquid column} \\
& \Rightarrow \text{ }W=T\times 2\pi r\times \dfrac{2T}{\rho rg} \\
& \Rightarrow \text{ }W=\dfrac{4\pi {{T}^{2}}}{\rho g} \\
\end{align}\]
So, we have the work done by the liquid to reach at height ‘h’ as –
\[W=\dfrac{4\pi {{T}^{2}}}{\rho g}\]
The correct answer is given by option B.
Note:
We can find the work done by integrating the surface tension over the area of contact, i.e., in this case the area of the circular face of the capillary tube. We had to find the height in this problem as the options involved didn’t have the height in the equation of the work done.
The work done by the liquid in rising in a capillary tube is the work done against the air pressure.
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